In [1]} the renormalization group equations were solved at \(Z_T \ne  0\) . The model has 2 complex scalar fields, the first components of the unconstrained superfields \(X\)  and \(T\) . A change of variables
\(Z_T\, T \bar{T}\rightarrow T { \bar{T}} \ , \qquad {1\over 2}TX^2 \rightarrow {1\over 2 \sqrt{Z_T} }TX^2 \ ,\) 
